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Quantum Yield and Mechanism of Singlet Oxygen Generation via UV Photoexcitation of O2–O2 and N2–O2 Encounter Complexes. / Пыряева, Александра Павловна; Goldort, Veniamin G.; Kochubei, Sergei A. et al.

In: The journal of physical chemistry. A, Vol. 116, No. 25, 04.06.2012, p. 6621-6629.

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Пыряева АП, Goldort VG, Kochubei SA, Бакланов АВ. Quantum Yield and Mechanism of Singlet Oxygen Generation via UV Photoexcitation of O2–O2 and N2–O2 Encounter Complexes. The journal of physical chemistry. A. 2012 Jun 4;116(25):6621-6629. doi: 10.1021/jp301471e

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Пыряева, Александра Павловна ; Goldort, Veniamin G. ; Kochubei, Sergei A. et al. / Quantum Yield and Mechanism of Singlet Oxygen Generation via UV Photoexcitation of O2–O2 and N2–O2 Encounter Complexes. In: The journal of physical chemistry. A. 2012 ; Vol. 116, No. 25. pp. 6621-6629.

BibTeX

@article{946dbf637e0d4fc3ad5e2405bdf9f266,
title = "Quantum Yield and Mechanism of Singlet Oxygen Generation via UV Photoexcitation of O2–O2 and N2–O2 Encounter Complexes",
abstract = "The mechanism and spectral dependence of the quantum yield of singlet oxygen O 2(a 1Δ g) photogenerated by UV radiation in gaseous oxygen at elevated pressure (32-130 bar) have been experimentally investigated within the 238-285 nm spectral region overlapping the range of the Wulf bands in the absorption spectrum of oxygen. The dominant channel of singlet oxygen generation with measured quantum yield up to about 2 is attributed to the one-quantum absorption by the encounter complexes O 2-O 2. This absorption gives rise to oxygen in the Herzberg III state O 2(A′ 3Δ u), which is assumed to be responsible for singlet oxygen production in the relaxation process O 2(A′ 3Δ u, ν) + O 2(X 3Σg-) → O 2({a 1Δ g}, {b 1Σg +}) + O 2({a 1Δ g, ν = 0}, {b 1Σg +, ν = 0}) with further collisional relaxation of b to a state. This mechanism is deduced from the analysis of the avoiding crossing locations on the potential energy surface of colliding O 2-O 2 pair. The observed drop of the O 2(a 1Δ g) yield near spectral threshold for O 2 dissociation is explained by the competition between above relaxation and reaction giving rise to O 3 + O (O + O + O 2) supposed in literature. The quantum yield of O 2(a 1Δ g) formation from encounter complex N 2-O 2 measured at λ = 266 nm was found to be the same as that for O 2-O 2.",
author = "Пыряева, {Александра Павловна} and Goldort, {Veniamin G.} and Kochubei, {Sergei A.} and Бакланов, {Алексей Васильевич}",
note = "The financial support of this work by Russian Foundation for Basic Research (09-03-00310-a) is gratefully acknowledged. APT thanks also ″OPTEC″ company for the financial support.",
year = "2012",
month = jun,
day = "4",
doi = "10.1021/jp301471e",
language = "English",
volume = "116",
pages = "6621--6629",
journal = "Journal of Physical Chemistry A",
issn = "1089-5639",
publisher = "American Chemical Society",
number = "25",

}

RIS

TY - JOUR

T1 - Quantum Yield and Mechanism of Singlet Oxygen Generation via UV Photoexcitation of O2–O2 and N2–O2 Encounter Complexes

AU - Пыряева, Александра Павловна

AU - Goldort, Veniamin G.

AU - Kochubei, Sergei A.

AU - Бакланов, Алексей Васильевич

N1 - The financial support of this work by Russian Foundation for Basic Research (09-03-00310-a) is gratefully acknowledged. APT thanks also ″OPTEC″ company for the financial support.

PY - 2012/6/4

Y1 - 2012/6/4

N2 - The mechanism and spectral dependence of the quantum yield of singlet oxygen O 2(a 1Δ g) photogenerated by UV radiation in gaseous oxygen at elevated pressure (32-130 bar) have been experimentally investigated within the 238-285 nm spectral region overlapping the range of the Wulf bands in the absorption spectrum of oxygen. The dominant channel of singlet oxygen generation with measured quantum yield up to about 2 is attributed to the one-quantum absorption by the encounter complexes O 2-O 2. This absorption gives rise to oxygen in the Herzberg III state O 2(A′ 3Δ u), which is assumed to be responsible for singlet oxygen production in the relaxation process O 2(A′ 3Δ u, ν) + O 2(X 3Σg-) → O 2({a 1Δ g}, {b 1Σg +}) + O 2({a 1Δ g, ν = 0}, {b 1Σg +, ν = 0}) with further collisional relaxation of b to a state. This mechanism is deduced from the analysis of the avoiding crossing locations on the potential energy surface of colliding O 2-O 2 pair. The observed drop of the O 2(a 1Δ g) yield near spectral threshold for O 2 dissociation is explained by the competition between above relaxation and reaction giving rise to O 3 + O (O + O + O 2) supposed in literature. The quantum yield of O 2(a 1Δ g) formation from encounter complex N 2-O 2 measured at λ = 266 nm was found to be the same as that for O 2-O 2.

AB - The mechanism and spectral dependence of the quantum yield of singlet oxygen O 2(a 1Δ g) photogenerated by UV radiation in gaseous oxygen at elevated pressure (32-130 bar) have been experimentally investigated within the 238-285 nm spectral region overlapping the range of the Wulf bands in the absorption spectrum of oxygen. The dominant channel of singlet oxygen generation with measured quantum yield up to about 2 is attributed to the one-quantum absorption by the encounter complexes O 2-O 2. This absorption gives rise to oxygen in the Herzberg III state O 2(A′ 3Δ u), which is assumed to be responsible for singlet oxygen production in the relaxation process O 2(A′ 3Δ u, ν) + O 2(X 3Σg-) → O 2({a 1Δ g}, {b 1Σg +}) + O 2({a 1Δ g, ν = 0}, {b 1Σg +, ν = 0}) with further collisional relaxation of b to a state. This mechanism is deduced from the analysis of the avoiding crossing locations on the potential energy surface of colliding O 2-O 2 pair. The observed drop of the O 2(a 1Δ g) yield near spectral threshold for O 2 dissociation is explained by the competition between above relaxation and reaction giving rise to O 3 + O (O + O + O 2) supposed in literature. The quantum yield of O 2(a 1Δ g) formation from encounter complex N 2-O 2 measured at λ = 266 nm was found to be the same as that for O 2-O 2.

UR - https://www.mendeley.com/catalogue/cfb314d7-d4a1-39d6-b800-490313f84f4a/

U2 - 10.1021/jp301471e

DO - 10.1021/jp301471e

M3 - Article

VL - 116

SP - 6621

EP - 6629

JO - Journal of Physical Chemistry A

JF - Journal of Physical Chemistry A

SN - 1089-5639

IS - 25

ER -

ID: 56406632